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                                   gain sufficient thermal energy to overcome the energy barrier that
                                   prohibits the electrons from escaping. The higher the tempera-
                                   ture, the higher the number of electrons emitted. Tungsten is
                                   commonly chosen as the filament because it can withstand high
                                   temperature without melting. However, thermionic electron guns
                                   have relatively low brightness.
                                     On the other hand, the field emission electron gun relies on elec-
                                   trons emitted from a sharp tip upon the application of a high elec-
                                   tric field. It does not involve heating of a filament. Instead, when a
                                   high electric field is applied to the tip, electrons from the tip quan-
                                   tum mechanically tunnel through the energy barrier into the vac-
                                   uum. Typically the field emission gun has two anodes. The first
                                   anode (at ∼0–5 kV) serves to extract the electrons from the tip,
                                   while the second anodes (at ∼1–50kV) serves to accelerate the
                                   electrons and this determines the energy of the electrons travel-
                                   ing down the column of the SEM. The field emission electron gun
                                   has a higher brightness.
                                     As the electrons are streaming out from the electron guns, they
                                   form a spray pattern. In order to control the profile of this electron
                                   beam into a finely adjusted focused beam, electromagnetic lenses
                                   are used. When an electron with charge q and velocity ~v travels
                                                                                           ~
                                                                  ~
                                   in a region with a magnetic field B, it will experience a force F
                                   given by:
                                                                   ~
                                                           ~
                                                           F = q~v × B
                                                                                         (8.3)
                                   One thing to note is that since the direction of the force is acting
                                   perpendicular to the direction of the velocity, the Lorentz force
                                   acting on the electrons has no effect on the speed of the electron.
                                   The only effect the magnetic field has on the electron is to change  ch08
                                   the direction of motion of the electrons.
                                     As shown in Fig. 8.7, the magnetic field profile generated by a
                                   typical electromagnet used in a SEM is highly non-uniform. The
                                   magnetic field of the electromagnetic lens can be considered to
                                   be made up of two independent components, the vertical axial
                                   component (Hz) and the horizontal radial component (Hr). The
                                   radial component causes the electron traveling in the −z direction
                                   to move in a helical manner with respect to the central axis. The
                                   axial component causes the electron to move closer to the central
                                   axis, i.e., the effect of the axial component is to reduce the diameter
                                   of the helical path of the electrons. As a result, the electron beam
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